Undergrad How to Understand the Primordial Power Spectrum in TASI Lectures on Inflation?

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SUMMARY

The discussion centers on understanding the Primordial Power Spectrum as presented in the TASI Lectures on Inflation by William Kinney. Key points include the derivation of the normalization constant ##\sqrt{-kτ}##, the order of the Bessel function ##ν##, and the simplification of the mode function to equation (166). Participants emphasize the importance of comparing equation (162) with the Bessel equation and utilizing spherical coordinates for angular integration in k-space to derive the power spectrum.

PREREQUISITES
  • Familiarity with the Klein-Gordon equation in expanding spacetime
  • Understanding of Bessel functions and their properties
  • Knowledge of Fourier analysis and its applications in cosmology
  • Basic concepts of spherical coordinates in k-space
NEXT STEPS
  • Study the derivation of the normalization constant in the context of the Klein-Gordon equation
  • Research the properties and applications of Bessel functions of order 3/2
  • Explore the two-point correlation function in cosmology
  • Read "Fundamentals of Cosmology" by James Rich, focusing on pages 248-252 and 258 for additional context
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Students and researchers in cosmology, particularly those studying inflationary theory and the mathematical tools used in analyzing the Primordial Power Spectrum.

Figaro
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I have been reading the TASI Lectures on Inflation by William Kinney, (https://arxiv.org/pdf/0902.1529v2.pdf).
I came across the mode function eq (128) (which obeys a generalization of the Klein-Gordon equation to an expanding spacetime), as I read through until eq (163), I know that it is the Hankel function (though he said it is the bessel function to which it is the solution to the differential equation in eq (162)),

1) How did he get the normalization constant ##\sqrt{-kτ}##?
2) How can I get the order of the Bessel function ##ν##?
3) How did he simplify the mode function to eq (166)?
 
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Figaro said:
I have been reading the TASI Lectures on Inflation by William Kinney, (https://arxiv.org/pdf/0902.1529v2.pdf).
I came across the mode function eq (128) (which obeys a generalization of the Klein-Gordon equation to an expanding spacetime), as I read through until eq (163), I know that it is the Hankel function (though he said it is the bessel function to which it is the solution to the differential equation in eq (162)),

1) How did he get the normalization constant ##\sqrt{-kτ}##?
2) How can I get the order of the Bessel function ##ν##?
3) How did he simplify the mode function to eq (166)?
Compare eq. 162 with the Bessel equation and read off nu and the normalization from there. The mode eq 166 results from the fact that Bessel functions of order 3/2 reduce to sines and cosines.
 
bapowell said:
Compare eq. 162 with the Bessel equation and read off nu and the normalization from there. The mode eq 166 results from the fact that Bessel functions of order 3/2 reduce to sines and cosines.
If I compare it, I'm just getting ##ν = \frac{\sqrt{2-ε}}{1-ε}##.
 
Hrm. Can you write down here the Bessel equation against which you are comparing Eq. 162?
 
bapowell said:
Hrm. Can you write down here the Bessel equation against which you are comparing Eq. 162?
##τ^2 u''_k + τ u'_k + ( τ^2 - p^2 ) u_k = 0##

Are there any other forms? I thought this is the form of the Bessel differential equation?
 
Sure. By changing the "time" variable, you can get rid of the u'_k term, for example. You need to do this in order to compare with Eq. 162, which has no first-order term.
 
bapowell said:
Sure. By changing the "time" variable, you can get rid of the u'_k term, for example. You need to do this in order to compare with Eq. 162, which has no first-order term.
Yes, I compared it with the bessel equation without the first order term. But I have solved my question 2 by using an alternate form of the bessel equation which I found in Boas's book eq 16.1. But I'm yet to solve my other questions.
 
For question 3, look up the Bessel functions of order 3/2. How are they written?
 
bapowell said:
For question 3, look up the Bessel functions of order 3/2. How are they written?
Sorry for the late reply because my laptop was broken. So, I have already worked out my questions but I have another question on equation (173), I can't find out how the power spectrum was derived. I mean, I don't know how he got from the first integral of (172) to the second integral.
 
  • #10
Figaro said:
I don't know how he got from the first integral of (172) to the second integral.

Assume spherical symmetry in k-space, change to spherical coordinates in k-space, and do the angular integration.
 
  • #11
George Jones said:
Assume spherical symmetry in k-space, change to spherical coordinates in k-space, and do the angular integration.
Before that, where can I read more about the two point correlation function? How about how to transform to Fourier space? I'm still new to this since I've just finished Cal I-III , DE and LA. Boas's treatment of Fourier analysis is way too basic so I haven't encountered those things. I'm really having a hard time understanding this lecture notes on Inflation. What do you recommend I should do/read to supplement this lecture notes? The latter part of Kinney's notes are very hard to understand, he skips a lot of details.
 
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  • #12
Figaro said:
Before that, where can I read more about the two point correlation function? How about how to transform to Fourier space?

You might try the second edition of "Fundamentals of Cosmology" by James Rich, pages 248 - 252, 258.

https://www.amazon.com/dp/3642425747/?tag=pfamazon01-20
 
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  • #13
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